Polyelectrolyte theory and chromatin-DNA quaternary structure: role of ionic strength and H1 histone

Complex formation in mixtures of lysozyme-stabilized emulsions and human saliva

In this paper, we studied the interaction between human unstimulated saliva and lysozyme-stabilized oil-in-water emulsions (10 wt/wt% oil phase, 10 mM NaCl, pH 6.7), to reveal the driving force for flocculation of these emulsions. Confocal scanning laser microscopy (CSLM) showed formation of complexes between salivary proteins and lysozyme adsorbed at the oil-water interface and lysozyme in solution as well. To assess the electrostatic nature of the interaction in emulsion/saliva mixtures, laser-diffraction and rheological measurements were conducted in function of the ionic strength by adding NaCl to the mixture in the range between 0 and 168 mM. Increasing the ionic strength reduced the ability of saliva to induce emulsion flocculation as shown by the decreased floc size and the effect on the viscosity. Turbidity experiments with varying pH (3-7) and ionic strength also showed decreased complex formation in mixtures between saliva and lysozyme in solution upon NaCl addition up to 200 mM. Decreasing the pH increased the turbidity, in line with the increase of the positive net charge on the lysozyme molecule. We conclude that electrostatic attraction is the main driving force for complex formation between saliva components and lysozyme adsorbed at the oil droplets and in solution.

X-ray small angle scattering study of chromatin as a function of fiber length

This work investigates the structure of native calf thymus chromatin as a function of fiber length and isolation procedures by using X-ray small angle scattering technique. Two methods of chromatin isolation have been compared in order to better understand the differences reported by various authors in terms of chromatin high order structure. In addition to these experimental results the effects of shearing have also been studied. In order to explain the differences among these chromatin preparations we built several models of chromatin fibers (represented as a chain of spherical subunits) assuming increasing level of condensation at increasing salt concentrations. For all these fiber models the corresponding theoretical X-ray scattering curves have been calculated and these results have been used to explain the influence of fiber length on the scattering profiles of chromatin. The comparison between experimental and theoretical curves confirms that the high molecular weight chromatin-DNA prepared by hypotonic swelling of nuclei (without enzymatic digestion) displays a partially folded structure even at low ionic strength, whereas the low molecular weight chromatin-DNA prepared by a brief nuclease digestion appears very weakly folded at the same ionic conditions.

DNA internal motions within nucleosomes during the cell cycle and as a function of ionic strength

We have used 31P NMR spectra to show that DNA internal motions are greatly hindered within oligonucleosomes. The fluctuations seem to be a function of both the cell cycle and the number of nucleosomes interlinked. Namely, the resonance areas, directly related to unbound phosphate, are consistently smaller in M-phase than in S-phase; at the same time, the resonance line width, inversely related to base plane, deoxyribose, and phosphate internal motions, is consistently larger in mononucleosomes than in oligonucleosomes. In all cases, the removal of chromosomal proteins, by a progressive increase of ionic strength up to 2 M NaCl, increases the internal motion, as monitored by a decrease in line width toward that of free DNA. While for both oligo- and mononucleosomes in S-phase the decrease in line width is strictly correlated to a sharp increase in resonance area, in M-phase it is not, with the 31P resonance area rather low even at 2.0 M NaCl extraction. Similarly, while S-phase 31P line widths steadily grow from mono- to oligonucleosomes, in M-phase they do not. Moreover, the increase of the ionic strength to 0.6 M NaCl, as compared to 0.35, 1.2, and 2 M NaCl, displays significant variations on 31P line width and resonance area, independent of the cell cycle phase and the number of nucleosomes interlinked. These observations agree with earlier suggestions on the differential role of the various chromosomal protein subfractions, known to preferentially dissociate at the different ionic strengths in question, in the sealing of mononucleosomes and in the overall stability of polynucleosomes.

Histone H1-DNA interactions and their relation to chromatin structure and function

The belief that histone H1 interacts primarily with DNA in chromatin and much less with the protein component has led to numerous studies of artificial H1-DNA complexes. This review summarizes and discusses the data on different aspects of the interaction between the linker histone and naked DNA, including cooperativity of binding, preference for supercoiled DNA, selectivity with respect to base composition and nucleotide sequence, and effect of H1 binding on the conformation of the underlying DNA. The nature of the interaction, the structure of the complexes, and the role histone H1 exerts in chromatin are also discussed.

Direct detection of linker DNA bending in defined-length oligomers of chromatin

Linker DNA, which connects between nucleosomes in chromatin, is short and, therefore, may be essentially straight and inflexible. We have carried out hydrodynamic and electron microscopic studies of dinucleosomes--fragments of chromatin containing just two nucleosomes--to test the ability of linker DNA to bend. We find that ionic conditions that stabilize the folding of long chromatin cause linker DNA in dinucleosomes to bend, bringing the two nucleosomes into contact. The results uphold a key prediction of the solenoid model of chromosome folding and suggest a mechanism by which proteins that are separated along the DNA can interact by direct contact.

Electrostatic mechanism of chromatin folding

We describe a theoretical analysis of cation binding in the nucleosome, and in chromatin as it folds, using Manning's polyelectrolyte theory. The theory accounts remarkably well, even quantitatively, both for the interaction of histone charges with DNA in chromatin, and for the essential features of the folding process. The degree of chromatin folding under different ion conditions is reliably predicted by the electrostatic free energy of DNA in the H1 binding site, which determines repulsions between linker DNA segments thus limiting how closely they may approach. The electrostatic free energy is a function of the ionic strength and the residual (unneutralized) DNA charge. Monovalent cations effect chromatin folding primarily by screening the residual charge whilst divalent or trivalent cations bind to DNA reducing its residual charge. The binding of H1 to the linker DNA considerably reduces its electrostatic free energy by displacing bound cations and reducing the residual charge. Thus, native chromatin folds at lower salt concentrations than does H1-depleted chromatin. We conclude that the mechanism of chromatin folding is primarily electrostatic in nature. In vivo ion conditions are such that chromatin is compact but H1 molecules are able to exchange freely, probably due to a low degree of salt-induced dissociation. When H1 molecules exchange, transient local disruptions may occur in the chromatin filament due to repulsion of temporarily H1-free linker DNA from within the filament, such that chromatin "breathes". Thus, the cell can maintain its chromatin in a compact form and access to DNA for sequence-specific DNA-binding proteins and the transcription machinery is still possible.

Native chromatin and damage induced by nuclease

Differential scanning calorimetry, gel electrophoresis and polarized light scattering of chromatin prepared by different methods have been carried out at low and high ionic strength, before and after shearing. These noninvasive studies, when compared to the ones similarly conducted in the corresponding native nuclei, conclusively point to the artefactual nature of chromatin prepared by limited nuclease digestion, which has no resemblence with the in situ chromatin-DNA structure being instead preserved by lysis of native nuclei and by subsequent sedimentation and suspension of the viscous chromatin mass. Native nucleofilaments appear longer than 200 nucleosomes and yield, from thermodynamic and optical standpoints, a tight quaternary structure maintained even at 0.01 M.

Condensation of the chromatin gel by cations

Calf thymus chromatin gel, containing strongly bound nonhistone proteins, was used to study the effect of easily removable and tightly bound cations on the condensation of chromatin. The chromatin volume was found to be linearly dependent on the reciprocal square root of the concentration of easily removable cations (Tris X H+ + Na+ and Mg2+) except for the initial stages of condensation (up to 7-10 mM monovalent and 0.15-0.2 mM divalent cations). The effect of Mg2+ at the initial stage of condensation was not reproduced by Na+ and vice versa. At higher concentrations the effects of Na+ and Mg2+ were additive. The removal of tightly bound divalent cations by a treatment of the chromatin gel with 1,10-phenanthroline led to an approx. 50% increase in the volume of the chromatin gel, which was maintained at each concentration of easily removable cations. The 1,10-phenanthroline-caused decondensation of the chromatin gel was reversed by Ca2+ but not by Mg2+, Zn2+ and Cu2+. The chromatin gel pretreated with Ca2+ was not further decondensed by 1,10-phenanthroline.

Packaged DNA. An elastic model

We review and deepen a theory of elastic bending of DNA on a persistence length scale. In a regime of extensive charge neutralization the axis of the double helix is elastically unstable when straight. Its stable bent conformation allows nucleation of DNA toruses and in principle could direct the supercoiled (solenoid) form of a polynucleosome. The Euler theory of elastic instability of macroscopic rods gives a partial description of the intrinsic ability of DNA to form locally stable bends. A different, quasi-Eulerian theory can be based on what is probably the dominant bending mechanism of DNA in solution-flexible kinking at the sites of open base pairs. This predictive theory is in quantitative agreement with the observed value (about 16 nm) for the minimum radius of torus holes. Stability of the inner torus ring is achieved when DNA phosphate groups are about 90% neutralized by trivalent cations, another prediction that is consistent with the observed formation of toruses in these conditions. The predicted stable radius of curvature of charge-neutralized DNA is also equal to the radial dimension of a maximally contracted polynucleosome supercoil as measured by neutron scattering (17 nm), but further experimental investigation of the geometrical disposition of the spacer DNA regions in the solenoid will be necessary to rule out the possibility of accidental agreement for this complex system. We stress again the experimental reality and probable importance of open base pairs in the equilibrium solution conformation of DNA.

Phase transitions in nuclei and chromatin. Is nuclear volume controlled by the chromatin or by the nuclear matrix?

Changes in the volume of rat liver nuclei have been monitored as a function of modifications in ionic environment (from 0 to 20 mM), temperature (from 4 to 37 degrees C), and pH (from 1 to 8). An abrupt reduction of nuclear volume occurred with increasing ion concentration, this contraction being more pronounced with bivalent (either Ca2+ or Mg2+) than with monovalent (either Na+ or K+) cations. The lowering of pH produced a similar effect. Parallel changes in chromatin structure took place at the same time as phase-like transitions. Atomic absorption spectroscopy allowed determination of free and nuclei-bound ions, pointing to the presence of a sizeable number of free binding sites for chromatin-DNA even within intact nuclei. DNA-phosphate sites appear to be neutralized by ions strictly according to the size of the electric charge and polyelectrolyte theory. Partial digestion (by micrococcal nuclease) or simple breaks (by chemical carcinogens) of the chromatin-DNA fiber caused respectively elimination or reduction of the abrupt volume changes in the intact nuclei. The apparent role of chromatin structure versus nuclear matrix in determining the shape and volume of intact nuclei is briefly discussed.

Properties of DNA rosettes and their relevance to chromosome structure

We have studied the spreading conditions that lead to the formation of rosettes in DNA and chromatin preparations from the amphibians Bufo marinus and Bolitoglossa subpalmata and the bacterium Shigella. Both nuclear preparations and extensively deproteinized DNA produced rosettes. The longest fibers and the most symmetric rosettes were observed in amphibian nuclear spreadings. In this procedure purified nuclei were submitted immediately to Kleinschmidt spreading over various types of hypophase. Distilled-water hypophases were most conducive for rosette production or stability. Rosettes were observed with cytochrome C as the basic protein, but not with ribonuclease A and bovine serum albumin. We cannot prove that all rosettes are artifacts of the spreading procedure, but we believe that at least some result from the expansion of compact DNA doughnuts and other structures that are apparently formed in the presence of basic proteins in salt concentrations over 40 mM (Olins and Olins 1971; Manning 1979). The dilute hypophase requirements is explainable by the assumption that dilution and spreading effects unfold a compact precursor. Occasionally we have detected structures that appear to be intermediates in the process of doughnut unfolding and that illustrate a procedure that may give rise to rosettes.

Histone H1: ultracentrifugation studies of the effects of ionic strength and denaturants on the solution conformation

The conformation of histone H1 has been examined under native and denaturing conditions in the absence of DNA or chromatin. Sedimentation coefficients were determined for Histone H1 in 0.1 M KCl and in 6 M guanidine hydrochloride solutions at pH 7.4. The influence of ionic strength on the conformation of histone H1 has been determined by measurement of the sedimentation coefficient in tetramethylammonium chloride solutions of up to 2.5 M and extrapolated to infinite ionic strength. Results from these experiments suggest that the native conformation of histone H1 is very asymmetric in shape. The molecule is best described as a prolate ellipsoid with axes of 312 A (2a) and 16 A (2b) in low ionic strength media and also as a prolate ellipsoid with axes of 202 A (2a) and 20 A (2b) at high ionic strength or when associated with polyanions, e.g., DNA. Denaturation of histone H1 by guanidine hydrochloride was found to be completely reversible. In 6 M guanidine hydrochloride, the H1 molecule collapses to a sphere but the original extended conformation of the protein is readily restored on dialysis. This suggests rigid conformational requirements for the H1 molecule as incorporated into chromatin. The shape and dimensions for the H1 molecule at high ionic strength are not sufficiently conclusive to locate H1 in the chromatin structure. It is proposed, however, that viable models for chromatin architecture must be consistent with the histone H1 solution dimensions obtained here.

Quaternary and quinternary structures of native chromatin DNA in liver nuclei: differential scanning calorimetry

Differential scanning calorimetry of chromatin isolated from rat liver cells revealed three discrete thermal transitions whose temperatures and melting enthalpies depend on ionic strength in the range 0 to 600 millimolar NaCl. Intact nuclei showed a fourth thermal transition at a lower temperature and different melting enthalpies for the other three transitions still present at temperatures similar to those obtained in isolated chromatin. The data are discussed in terms of the tertiary, quaternary, and quinternary structures of chromatin DNA.